Choosing an energy \(\mu _0\)  above \(\Lambda _H\)  as a measurement probe of
the running of \(\lambda \)  is attempting to make a measurement within
the finite Gaussian distribution length size
\(\ell _H\)  [1]} and is prohibited within the perturbation
approximations we have assumed. The results obtained for the running
of \(\lambda \)  are for a single Higgs particle interacting with another
Higgs particle. This cannot describe a fully realistic situation, for
the Higgs coupling to other particles such as the top quark (the top
quark-Higgs coupling \(\lambda _t\sim {\cal O}(1)\) ) may play an
important role.
